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Re: [abinit-forum] Angular momentum decomposition of KS states.


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  • From: mmikami@rc.m-kagaku.co.jp
  • To: forum@abinit.org
  • Subject: Re: [abinit-forum] Angular momentum decomposition of KS states.
  • Date: Tue, 1 Jul 2003 10:39:17 +0900

Hi,

In passing, I would like to add one reference related to this topic:
N.V. Skorodumova et al., Phys.Rev B64, 115108 (2001)
Just take a look at the Fig.3, and read some paragraphs
that begin from page 115108-3 (In Fig.3 (DOS of CeO2),
the presence of some Ce d and f characters in the p band of O, ...)
From the viewpoint of Prof. Andersen et al,
"Ce d and f states found in the oxygen p band could be just
tails neighboring O electronic states spilling into the Ce MTS's."
In fact, the bonding nature in CeO2 appears polarized ionic
rather than covalent, from the result of electron localization
function (ELF).

Such situation may be common. For example, Al-d state in DOS
for compounds are also observed. It may come from the tails of
wavefunctions of the neighboring atom.

Masayoshi Mikami
------------------------------------------------------------------------ --
Masayoshi Mikami, Ph.D
------------------------------------------------------------------------ --
Mitsubishi Chemical Group Science and Technology Research Center, Inc.
Address: 1000, Kamoshida-cho Aoba-ku, Yokohama, 227-8502, Japan
Phone: +81-45-963-3834 Fax: +81-45-963-3835
E-mail: mmikami@rc.m-kagaku.co.jp
------------------------------------------------------------------------ --

On 2003.7.1, at 03:25 Asia/Tokyo, Allan, Douglas C Dr wrote:

Also, think of any given eigenstate as having arbitrarily many angular momentum components (for reasons that Jim described). The angular momentum decomposition is simply a representation of the arbitrary eigenstate into components that each transform according to the various spherical harmonics, each of which has a definite eigenvalue under rotations. Jim's is the more physical answer, but also keep in mind that any arbitrary wave function can be written as a sum of terms that are eigenstates of rotation (i.e. spherical harmonics).

To test abinit and your understanding, you can try calculating a single atom in a large box and see whether the angular momentum decomposition looks right to you. If the box is too small then periodic image atoms can perturb the results a little.

Of course, there is always the small chance that a bug may exist, so such tests are worthwhile for your confidence and for the continued improvement of the code ...

Doug Allan

-----Original Message-----
From: James Raynolds [mailto:JRaynolds@uamail.albany.edu]
Sent: Monday, June 30, 2003 8:41 AM
To: 'forum@abinit.org'
Subject: RE: [abinit-forum] Angular momentum decomposition of KS states.


Fabrizio,

Placing the atom in the solid lowers the symmetry and so you can get all these other components due to interactions with the other atoms.

Jim Raynolds

-----Original Message-----
From: Fabrizio Cleri [mailto:cleri@casaccia.enea.it]
Sent: Monday, June 30, 2003 7:03 AM
To: forum@abinit.org
Subject: [abinit-forum] Angular momentum decomposition of KS states.


Hi,
we are doing some angular decomposition of wavefunctions in molecules
based on the ABINIT capabilities discussed below...
however, I have some basic doubt: what does it mean the d, f, g
component when I start from atoms which have only s and/or p electrons?
In some cases we found C atoms with the f component being the 90% of
the wf for a particular k and band...

thanks for your patience,
F. Cleri



Inizio del messaggio inoltrato:

Da: verstraete@pcpm.ucl.ac.be
Data: Gio 30 Gen 2003 18:00:13 Europe/Rome
A: forum@abinit.org
Cc: balkagl@sancharnet.in
Oggetto: [abinit-forum] angular momentum decomposition of KS states.
Rispondere-A: verstraete@pcpm.ucl.ac.be

In answer to the mail below, a brief explanation of what you can now
do to
analyse the s, p, d, character of a given state:

If cut3d is called, and a _WFK file is entered instead of a _DEN file,
you
get a menu for the analysis of the different electronic states.

If appropriate (ie. more than 1 choice) you can choose a kpoint, a
band, a
spin polarisation, and (4.0.3?) a spinorial component.

cut3d extracts the appropriate wavefunction, and asks you if you want
to
do its angular analysis. Typing 1 (yes) here will do the analysis:
for each atom, the wavefunction surrounding the atom will be projected
into s, p, d, f, and g components. The output is the relative
percentage
of spdfg, for each atom, and then globally for the state. The
projection
is fast, but depends on your cutoff energy, so for 100s of bands it can
take a few minutes or even a 1/4 an hour.

Afterwards, type 12 to exit the next menu (other operations on the
wavefunction), and 1 if you want a new state to analyse. Otherwise 2
to exit. Simple, hmmm?

This process is still fairly painful if you don't script it (simple
enough
since cut3d reads from stdout) to loop over kpts and bands. I will in
future combine this to give you angular momentum decomposition of the
DOS,
but as yet I don't see any relativistic effects on my time, so we'll
have
to wait.


Matthieu

--
===================================================================
Matthieu Verstraete mailto:verstraete@pcpm.ucl.ac.be
PCPM, Boltzmann, pl. Croix du Sud, 1 tel: 010/ 47 86 81
B-1348 Louvain-la-Neuve Belgium fax: 010/ 47 34 52

---------- Forwarded message ----------
Date: Thu, 30 Jan 2003 16:05:43 +0100
From: Xavier Gonze <gonze@pcpm.ucl.ac.be>
To: Bal K. Agrawal <balkagl@sancharnet.in>
Cc: mverstra@pcpm.ucl.ac.be
Subject: Re: Abinit

Dear Bal K. Agrawal,

Bal K. Agrawal wrote:
Dear Prof. Gonze
In the Abinit code we want to know the contributions of atomic
orbitals to the electronic state of the system. Is it possible ? If
yes, please explain us.
with best regards.
Prof. B. K. Agrawal
Physics Department
Allahabad University
INDIA

I relay your demand to the appropriate person (Matthieu Verstraete,
who developed this for v4.0 , so this is very recent). Still, it would
be better to send such mail to forum@abinit.org , where all the
interested persons (both knowning the solution or interested to hear
about) will be contacted.

Good continuation,
Xavier Gonze







______________________________________
Fabrizio Cleri
ENEA, UTS Materiali e Nuove Tecnologie
Centro Ricerche Casaccia, s.p. 050
00100 Roma A.D., Italy
tel.: +39-06-30484825
fax: +39-06-30484729
e-mail: cleri@casaccia.enea.it
e-page: http://babylon.casaccia.enea.it/TMM.html






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